# Distances between elements (standardized)

Source:`vignettes/web/elements-distances-standardized.Rmd`

`elements-distances-standardized.Rmd`

### Introduction

As a similarity measure in grids different types of Minkowski metrics, especially the Euclidean and city-block metric are frequently used. The Euclidean distance is the sum of squared differences between the ratings on two different elements. They are, however, no standardized measure. The distances strongly depend on the number of constructs and the rating range. The figure below demonstrates this fact. Note how the distance changes although the rating pattern remains identical.

In order to be able to compare distances across grids of different
size and rating range a standardization is desireable. Also, the notion
of *significance of a distance*, i.e. a distance which is
unusually big, is easier with a standard reference measure. Different
suggestions have been made in the literature of how to standardize
Euclidean interelement distances (Hartmann, 1992;
Heckmann, 2012; Slater, 1977). The three variants will be briefly
discussed and the corresponing R-Code is demonstrated.

### Slater distances (1977)

#### Description

The first suggestion to standardization was made by Slater (1977). He essentially calculated an expected
average Euclidean distance \(U\) for
the case if the ratings are randomly distributed. To standardize the
grids he suggested to divide the matrix of Euclidean distances \(E\) by this *unit of expected
distance* \(U\). The Slater
standardization thus is the division of the Euclidean distances by the
distance expected on average. Hence, distances bigger than 1 are greater
than expected, distances smaller than 1 are smaller than expected.

#### R-Code

The function `distanceSlater`

calculates Slater distances
for a grid.

```
distanceSlater(boeker)
#
# ##########################
# Distances between elements
# ##########################
#
# Distance method: Slater (standardized Euclidean)
# Normalized:
# 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15
# (1) self 1 1.03 0.75 0.69 0.87 1.19 0.80 1.03 0.99 0.59 1.79 0.58 0.55 0.64 0.54
# (2) ideal self 2 1.11 0.78 1.06 1.31 1.07 0.97 1.14 0.97 1.56 1.22 1.21 1.24 1.25
# (3) mother 3 0.73 0.53 0.95 0.55 0.81 0.64 0.67 1.58 0.69 0.83 0.77 0.69
# (4) father 4 0.63 1.15 0.65 0.90 0.83 0.69 1.66 0.84 0.91 0.98 0.89
# (5) kurt 5 0.89 0.57 0.79 0.57 0.72 1.51 0.79 0.93 0.87 0.83
# (6) karl 6 0.94 0.74 0.66 1.09 0.97 1.17 1.22 1.08 1.15
# (7) george 7 0.92 0.65 0.81 1.51 0.73 0.91 0.92 0.78
# (8) martin 8 0.68 0.80 1.27 1.09 1.10 1.01 1.07
# (9) elizabeth 9 0.87 1.31 1.00 1.13 1.03 0.98
# (10) therapist 10 1.74 0.65 0.63 0.69 0.65
# (11) irene 11 1.83 1.86 1.72 1.84
# (12) childhood self 12 0.43 0.50 0.34
# (13) self before illness 13 0.43 0.41
# (14) self with delusion 14 0.45
# (15) self as dreamer 15
#
# Note that Slater distances cannot be compared across grids with a different number of constructs (see Hartmann, 1992).
```

You can save the results and define the way they are displayed using
the `print`

method. For example we could display distances
only within certain boundaries, using the `cutoff`

values
`.8`

and `1.2`

to indicate very big or small
distances as suggested by Norris and Makhlouf-Norris (1976).

```
d <- distanceSlater(boeker)
print(d, cutoffs=c(.8, 1.2))
#
# ##########################
# Distances between elements
# ##########################
#
# Distance method: Slater (standardized Euclidean)
# Normalized:
# 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15
# (1) self 1 0.75 0.69 0.80 0.59 1.79 0.58 0.55 0.64 0.54
# (2) ideal self 2 0.78 1.31 1.56 1.22 1.21 1.24 1.25
# (3) mother 3 0.73 0.53 0.55 0.64 0.67 1.58 0.69 0.77 0.69
# (4) father 4 0.63 0.65 0.69 1.66
# (5) kurt 5 0.57 0.79 0.57 0.72 1.51 0.79
# (6) karl 6 0.74 0.66 1.22
# (7) george 7 0.65 1.51 0.73 0.78
# (8) martin 8 0.68 0.80 1.27
# (9) elizabeth 9 1.31
# (10) therapist 10 1.74 0.65 0.63 0.69 0.65
# (11) irene 11 1.83 1.86 1.72 1.84
# (12) childhood self 12 0.43 0.50 0.34
# (13) self before illness 13 0.43 0.41
# (14) self with delusion 14 0.45
# (15) self as dreamer 15
#
# Note that Slater distances cannot be compared across grids with a different number of constructs (see Hartmann, 1992).
```

#### Calculation

Let \(G\) be the raw grid matrix and \(D\) be the grid matrix centered around the construct means, with \(d_{ij} =g_{..} - g_{ij}\), where \(g_{..}\) is the mean of the construct. Further, let

\[P=D^TD \qquad \text{and} \qquad S=tr\;P\]

The Euclidean distances results in:

\[(\sum{ (d_{ij} - d_{ik} )^2})^{1/2}\]

\[\Leftrightarrow (\sum{ (d_{ij}^2 + d_{ik}^2 - 2d_{ij}d_{ik})})^{1/2}\]

\[\Leftrightarrow (\sum{ d_{ij}^2 } + \sum{d_{ik}^2} - 2\sum{d_{ij}d_{ik} })^{1/2}\]

\[\Leftrightarrow (S_j + S_k - 2P_{jk})^{1/2}\]

For the standardization, Slater proposes to use the expected
Euclidean distance between a random pair of elements taken from the
grid. The average for \(S_j\) and \(S_k\) would then be \(S_{avg} = S/m\) where \(m\) is the number of elements in the grid.
The average of the off-line diagonals of \(P\) is \(S/m(m-1)\) (see
Slater, 1951, for a proof). Inserted into the formula above it
gives the following expected average euclidean distance \(U\) which is outputted as *unit of
expected distance* in Slater’s INGRID program.

\[U = (2S/(m-1))^{1/2}\]

The calculated euclidean distances are then divided by \(U\), the *unit of expected distance*
to form the matrix of standardized element distances \(E_{std}\), with

\[E_{std} = E/U\]

### Hartmann distances (1992)

#### Description

Hartmann (1992) showed in a Monte Carlo
study that Slater distances (see above) based on random grids, for which
Slater coined the expression *quasis*, have a skewed
distribution, a mean and a standard deviation depending on the number of
constructs elicited. Hence, the distances cannot be compared across
grids with a different number of constructs. As a remedy he suggested a
linear transformation (z-transformation) of the Slater distance values
which take into account their estimated (or alternatively expected) mean
and their standard deviation to standardize them. Hartmann distances
represent a more accurate version of Slater distances. Note that
Hartmann distances are multiplied by -1 to allow an interpretation
similar to correlation coefficients: negative Hartmann values represent
an above average dissimilarity (i.e. a big Slater distance) and positive
values represent an above average similarity (i.e. a small Slater
distance).

The *Hartmann distance* is calculated as follows (Hartmann, 1992, p. 49).

\[D = -1 \frac{D_{slater} - M_c}{sd_c}\]

Where \(D_{slater}\) denotes the Slater distances of the grid, \(M_c\) the sample distribution’s mean value and \(sd_c\) the sample distributions’s standard deviation.

#### R-Code

The function `distanceHartmann`

calculates Hartmann
distances. The function can be operated in two ways. The default option
(`method="paper"`

) uses precalculated mean and standard
deviations (as e.g. given in Hartmann
(1992)) for the standardization.

```
distanceHartmann(boeker)
#
# ##########################
# Distances between elements
# ##########################
#
# Distance method: Hartmann (standardized Slater distances)
# Normalized:
# 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15
# (1) self 1 -0.28 1.58 1.92 0.80 -1.33 1.20 -0.29 -0.04 2.62 -5.24 2.66 2.87 2.28 2.89
# (2) ideal self 2 -0.78 1.36 -0.47 -2.09 -0.56 0.12 -1.02 0.12 -3.69 -1.50 -1.45 -1.63 -1.71
# (3) mother 3 1.70 2.99 0.22 2.82 1.15 2.27 2.09 -3.84 1.91 1.06 1.44 1.92
# (4) father 4 2.31 -1.04 2.23 0.55 1.00 1.92 -4.39 0.96 0.50 0.08 0.63
# (5) kurt 5 0.63 2.72 1.27 2.69 1.74 -3.37 1.30 0.35 0.79 1.01
# (6) karl 6 0.29 1.63 2.14 -0.66 0.10 -1.21 -1.53 -0.60 -1.04
# (7) george 7 0.45 2.19 1.17 -3.39 1.70 0.54 0.42 1.35
# (8) martin 8 2.03 1.22 -1.85 -0.67 -0.73 -0.13 -0.53
# (9) elizabeth 9 0.76 -2.07 -0.08 -0.91 -0.29 0.05
# (10) therapist 10 -4.91 2.20 2.35 1.97 2.22
# (11) irene 11 -5.47 -5.65 -4.79 -5.52
# (12) childhood self 12 3.66 3.16 4.22
# (13) self before illness 13 3.60 3.79
# (14) self with delusion 14 3.52
# (15) self as dreamer 15
#
# For calculation the parameters from Hartmann (1992) were used. Use 'method=new' or method='simulate' for a more accurate version.
```

The second option (`method="simulate"`

) is to simulate the
distribution of distances based on the size and scale range of the grid
under investigation. A distribution of Slater distances is derived using
quasis and used for the Hartmann standardization instead of the
precalculated values. The following simulation is based on
`reps=1000`

quasis.

```
h <- distanceHartmann(boeker, method="simulate", reps=1000)
h
```

```
#
# ##########################
# Distances between elements
# ##########################
#
# Distance method: Hartmann (standardized Slater distances)
# Normalized:
# 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15
# (1) self 1 -0.28 1.56 1.90 0.79 -1.32 1.19 -0.29 -0.04 2.59 -5.19 2.63 2.84 2.25 2.86
# (2) ideal self 2 -0.77 1.35 -0.47 -2.07 -0.56 0.12 -1.01 0.12 -3.65 -1.48 -1.43 -1.62 -1.70
# (3) mother 3 1.68 2.96 0.21 2.79 1.14 2.25 2.07 -3.80 1.89 1.04 1.42 1.90
# (4) father 4 2.28 -1.04 2.20 0.54 0.99 1.90 -4.35 0.95 0.49 0.08 0.62
# (5) kurt 5 0.62 2.69 1.25 2.66 1.72 -3.34 1.28 0.34 0.78 0.99
# (6) karl 6 0.28 1.61 2.11 -0.65 0.09 -1.20 -1.51 -0.59 -1.03
# (7) george 7 0.44 2.17 1.15 -3.36 1.68 0.53 0.41 1.33
# (8) martin 8 2.01 1.20 -1.83 -0.67 -0.73 -0.13 -0.52
# (9) elizabeth 9 0.75 -2.05 -0.08 -0.90 -0.28 0.05
# (10) therapist 10 -4.86 2.18 2.32 1.95 2.19
# (11) irene 11 -5.41 -5.59 -4.74 -5.46
# (12) childhood self 12 3.62 3.12 4.18
# (13) self before illness 13 3.56 3.75
# (14) self with delusion 14 3.48
# (15) self as dreamer 15
```

If the results are saved, there are a couple of options for printing
the object (see `?print.hdistance`

).

```
print(d, p=c(.05, .95))
#
# ##########################
# Distances between elements
# ##########################
#
# Distance method: Slater (standardized Euclidean)
# Normalized:
# 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15
# (1) self 1 1.03 0.75 0.69 0.87 1.19 0.80 1.03 0.99 0.59 1.79 0.58 0.55 0.64 0.54
# (2) ideal self 2 1.11 0.78 1.06 1.31 1.07 0.97 1.14 0.97 1.56 1.22 1.21 1.24 1.25
# (3) mother 3 0.73 0.53 0.95 0.55 0.81 0.64 0.67 1.58 0.69 0.83 0.77 0.69
# (4) father 4 0.63 1.15 0.65 0.90 0.83 0.69 1.66 0.84 0.91 0.98 0.89
# (5) kurt 5 0.89 0.57 0.79 0.57 0.72 1.51 0.79 0.93 0.87 0.83
# (6) karl 6 0.94 0.74 0.66 1.09 0.97 1.17 1.22 1.08 1.15
# (7) george 7 0.92 0.65 0.81 1.51 0.73 0.91 0.92 0.78
# (8) martin 8 0.68 0.80 1.27 1.09 1.10 1.01 1.07
# (9) elizabeth 9 0.87 1.31 1.00 1.13 1.03 0.98
# (10) therapist 10 1.74 0.65 0.63 0.69 0.65
# (11) irene 11 1.83 1.86 1.72 1.84
# (12) childhood self 12 0.43 0.50 0.34
# (13) self before illness 13 0.43 0.41
# (14) self with delusion 14 0.45
# (15) self as dreamer 15
#
# Note that Slater distances cannot be compared across grids with a different number of constructs (see Hartmann, 1992).
```

### Heckmann’s approach (2012)

#### Description

Hartmann (1992) suggested a transformation of Slater (1977) distances
to make them independent from the size of a grid. Hartmann distances are
supposed to yield stable cutoff values used to determine ‘significance’
of inter-element distances. It can be shown that Hartmann distances are
still affected by grid parameters like size and the range of the rating
scale used (Heckmann, 2012). The function
`distanceNormalize`

applies a Box-Cox (1964) transformation to the Hartmann distances
in order to remove the skew of the Hartmann distance distribution. The
normalized values show to have more stable and nearly symmetric cutoffs
(quantiles) and better properties for comparison across grids of
different size and scale range.

#### R-Code

The function `distanceNormalize`

will return Slater,
Hartmann or power transformed Hartmann distances (Heckmann, 2012) if prompted. It is also
possible to return the quantiles of the sample distribution and only the
element distances consideres ‘significant’ according to the quantiles
defined.

```
n <- distanceNormalized(boeker)
n
```

```
#
# ##########################
# Distances between elements
# ##########################
#
# Distance method: Power transformed Hartmann distances
# Normalized:
# 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15
# (1) self 1 -0.28 1.56 1.90 0.79 -1.32 1.19 -0.29 -0.04 2.59 -5.18 2.63 2.84 2.25 2.86
# (2) ideal self 2 -0.77 1.35 -0.47 -2.07 -0.56 0.12 -1.01 0.12 -3.65 -1.48 -1.43 -1.62 -1.70
# (3) mother 3 1.68 2.96 0.21 2.79 1.14 2.25 2.07 -3.80 1.89 1.04 1.42 1.90
# (4) father 4 2.28 -1.04 2.20 0.54 0.99 1.90 -4.34 0.94 0.49 0.08 0.62
# (5) kurt 5 0.62 2.69 1.25 2.66 1.72 -3.34 1.28 0.34 0.78 0.99
# (6) karl 6 0.28 1.61 2.11 -0.65 0.09 -1.19 -1.51 -0.59 -1.03
# (7) george 7 0.44 2.17 1.15 -3.36 1.68 0.53 0.41 1.33
# (8) martin 8 2.01 1.20 -1.83 -0.67 -0.73 -0.13 -0.52
# (9) elizabeth 9 0.75 -2.05 -0.08 -0.90 -0.28 0.05
# (10) therapist 10 -4.86 2.18 2.32 1.95 2.19
# (11) irene 11 -5.41 -5.59 -4.74 -5.46
# (12) childhood self 12 3.62 3.12 4.17
# (13) self before illness 13 3.56 3.75
# (14) self with delusion 14 3.48
# (15) self as dreamer 15
```

#### Calculation

The form of normalization applied by Hartmann (1992) does not account for skewness or kurtosis. Here, a form of normalization - a power transformation - is explored that takes into account these higher moments of the distribution. For this purpose Hartmann values are transformed using the ‘’Box-Cox’’ family of transformations (Box & Cox, 1964). The transformation is defined as

\[ Y_i^{\lambda}= \left\{ \begin{matrix} \frac{(Y_i + c)^\lambda - 1}{\lambda} & \mbox{for }\lambda \neq 0 \\ ln(Y_i + c) & \mbox{for }\lambda = 0 \end{matrix} \right. \]

As the transformation requires values \(\ge 0\) a constant \(c\) is added to derive positive values only. For the present transformation \(c\) is defined as the minimum Hartmann distances from the quasis distribution. In order to derive at a transformation that resembles the normal distribution as close as possible, an optimal \(\lambda\) is searched by selecting a \(\lambda\) that maximizes the correlation between the quantiles of the transformed values \(Y_i^\lambda\) and the standard normal distribution. As a last step, the power transformed values \(Y_i^\lambda\) are z-transformed to remove the arbitrary scaling resulting from the Box-Cox transformation yielding \(Y_i^P\).

\(Y_{i}^P = \frac{Y^{\lambda}_i - \overline Y^{\lambda}}{\sigma_{Y^{\lambda}}}\)

### Literature

*Journal of the Royal Statistical Society. Series B (Methodological)*,

*26*(2), 211–252. Retrieved from http://www.jstor.org/stable/2984418

*International Journal of Personal Construct Psychology*,

*5*(1), 41–56. doi:10.1080/08936039208404940

*The measurement of intrapersonal space by grid technique: Explorations of intrapersonal space*(Vol. 1, pp. 79–92). London: Wiley & Sons.

*British Journal of Statistical Psychology*,

*6*, 101–106.

*The measurement of intrapersonal space by grid technique: Dimensions of intrapersonal space*(Vol. 2). London: Wiley & Sons.